charm physics and xyz states at besiii
play

Charm physics and XYZ states at BESIII Evgeny BOGER JINR Dubna On - PowerPoint PPT Presentation

Charm physics and XYZ states at BESIII Evgeny BOGER JINR Dubna On behalf of BESIII collaboration FAIRNESS2016 Feb. 15, 2016 Charm + XYZ at BES-III Outline BESIII experiment Charm physics Recent XYZ results 2 Charm + XYZ at


  1. Charm physics and XYZ states at BESIII Evgeny BOGER JINR Dubna On behalf of BESIII collaboration FAIRNESS2016 Feb. 15, 2016 Charm + XYZ at BES-III

  2. Outline ● BESIII experiment ● Charm physics ● Recent XYZ results 2 Charm + XYZ at BES-III

  3. BEPC II LINAC e + e - BES-III 8 × 10 32 cm − 2 s − 1 Achieved luminocity: Beam energy: 1 - 2.3 GeV Beam current: 0.91A 3 Charm + XYZ at BES-III

  4. BESIII Detector 1T superconducting magnet EMC : CsI crystals ● Energy resolution: 2.5%@1GeV ● Spatial resulution: 6mm ● MDC : Spatial resulution: σ xy = 120μm ● Momentum resolution: 0.5%@1GeV ● dE/dx resolution: 6% ● TOF Two layers of scintillator ● Time resolution: ● 90 ps (barel), 120 ps (endcaps) Muon ID 8 layers of RPC inside the yoke ● (9 in endcaps) 4 Charm + XYZ at BES-III

  5. BESIII Data Sample Image from S. Spataro – Spectroscopy in the charm range: from BESIII to PANDA ● Data taking since 2008 ● World largest sample in e + e - → : J/ψ, ψ(2S), ψ(3770), Y(4260) 5 Charm + XYZ at BES-III

  6. Charm physics at BESIII: Motivation Unitarity test of CKM matrix: measuring |V cs | ● and |V cd | LQCD calibration: f D->K/π (q 2 ) and other FFs, f D(s)+ ● decay constant New Physics: fjnding evidence of CP violation, ● rare decays, signifjcant deviations from CKM unitarity or from LQCD calculations Providing inputs for b-physics ● 6 Charm + XYZ at BES-III

  7. Charm physics: data samples 0 D 0 , D + D − 1 @ 3.773 GeV for D - 2.93 fb + D s − 1 @ 4.009 GeV for D s - 0.48 fb − 1 @ 4.599 GeV for Λ c + Λ c - 0.57 fb 7 Charm + XYZ at BES-III

  8. Analysis Technique Pure DD fjnal state, no ● Example: e + e - → ψ(3770) → D D additional hadrons «Tag» D-meson is fully ● reconstructed Signal is searched at the ● recoiling side Tag selection based on two ● variables: m BC = √ E beam 2 Δ E = E D − E beam −| ⃗ p D | Tag yeild is obtained by fjtting ● m BC 8 Charm + XYZ at BES-III

  9. Analysis of D + → K - π + e + ν e Branching fractions arxiv:1512.08627 ● BESIII preliminary ● Amplitude analysis BESIII preliminary Fitted fractions (S+P) – BESIII preliminary S-wave phase measurement ● N sig = 18262 Consistent with LASS parameterization – background level: 0.7% Model-independent helicity basis FF study ● Consistent with the PWA solution and CLEO-c – results Cont. 9 Charm + XYZ at BES-III

  10. PWA of D + → K - π + e + ν e Projections of data and PWA solution MC (S+P) BESIII preliminary BESIII preliminary First measurement of SPD V pole mass 10 arxiv:1512.08627 Charm + XYZ at BES-III

  11. D + → K - π + e + ν e S-wave phase S-wave phase δ s is independently fjtted in 12 m Kπ bins BESIII preliminary Blue dots: BESIII model-independent measurement Red and dotted lines: predicted by fjt based on LASS parameterization Green dots: BABAR model-independent measurement with S+D+P Model-independent measurement of BESIII are consistent with its result from amplitude analysis within 1σ . 11 arxiv:1512.08627 Charm + XYZ at BES-III

  12. Model-Independent Measurement of Form Factors • Events located in the K * window [0.8,1] GeV/c 2 , are used to measure the form factors by a Projective Weighting Technique [Phys. Rev. D 81, 112001 (2010)]. • Signal is assumed to be composed of K* and a non-resonant S-wave. • Helicity basis form factors include: P-wave related: H ± (q 2) ● BESIII preliminary S-wave related: h 0 (q 2 ) ● Five weighted q 2 histograms are built. ● Weight is assigned to each event based on kinematic variables. Form factors are independently computed ● in each bin. Red dots : BESIII model-independent measurement The model-independent measurements ● Black dots : CLEO model-independent measurement are generally consistent with CLEO-c and Blue Line : BESIII result from amplitude analysis (it's not the fjt!) with SPD-model results from amplitude analysis 12 arxiv:1512.08627 Charm + XYZ at BES-III

  13. Study of D 0 → K - /π - e + ν e Using CKMFitter |V cs(d) | as input Measure |V cs(d) | × f + PRD92 (2015) 072012 K( π) D 0 → K - e + ν e D 0 → π - e + ν e 13 Charm + XYZ at BES-III

  14. Study of D + → ωe + ν e and search for D + → ϕ e + ν e First D + → ωe + ν e form factor D + → ωe + ν e measurement PRD 92, 071101(R) (2015) D + → ϕ e + ν e data Form factor ratios: Branching ratios: 14 Charm + XYZ at BES-III

  15. Observation of D + → ωπ + and evidence for D 0 → ωπ 0 D + → ωπ + is singly Cabibbo-suppressed arXiv:1512.06998 D + → ωπ + D 0 → ωπ 0 4.1σ BESIII preliminary 5.5σ BESIII preliminary BESIII preliminary 15 Charm + XYZ at BES-III

  16. Absolute BF for Λ + c →Λ e + ν e 109.4±10.9 ST + →Λ e + ν e ) BF (Λ c Theoretical predictions: 1.4% to 9.2% Previous indirect measurements: ( 2.9 ± 0.5 ) % First direct measurement + →Λ e + ν e )=( 3.63 ± 0.38 ± 0.20 ) % BF (Λ c PRL115(2015)221805 16 Charm + XYZ at BES-III

  17. XYZ States “XYZ” states: ● Charmonium (cc) in the fjnal state ● Do not fjt into the conventional quark model of charmonium Image from S. Olsen Front. Phys. 10, 101401 (2015) 17 Charm + XYZ at BES-III

  18. Exotic Hadrons ● Conventional hadrons: 2 or 3 quarks ● QCD doesn't forbid exotic hadrons: ● Glueball (no quarks) ● Hybrid (quarks + excited gluon) ● Multiquark (N > 3) ● Hardon molecule (bound state of hadrons) 18 Charm + XYZ at BES-III

  19. BESIII Data Sets 19 Charm + XYZ at BES-III

  20. Z c states at BESIII Neutral partner is found Z c (3900) + in e + e - → π + π - J/ψ Z c (3900) 0 Charged charmonium-like state ● M = (3899.0 ± 3.6 ± 4.9) MeV/c 2 ● Γ = (46 ± 10 ± 20) MeV/c 2 ● Signifjcance > 8σ M = 3894.8 ± 2.3 ± 3.2 MeV/c 2 ● Γ = 29.6 ± 8.2 ± 8.2 MeV/c 2 ● Significance = 10.4σ ● Isospin triplet PRL 115, 112003 (2015) 20 PRL110, 252001[2013] Charm + XYZ at BES-III

  21. Z c states at BESIII Z c (3885) + Found in e + e - → π + (DD * ) - @ 4.26 GeV (ST) confjrmed @ 4.23, 4.26 GeV (DT) M = 3881.7 ± 1.6 ± 2.1 MeV/c 2 ● Γ = 26.6 ± 2.0 ± 2.3 MeV/c 2 ● Signifjcance > 10σ ● Angular distribution consistent with ● J P =1 + Isospin triplet PRD 92, 092006 (2015) Z c (3885) 0 e + e - → π 0 (DD * ) 0 M = 3885.7 +4.3 -5.7 ± 8.4 MeV/c 2 ● Γ = 35 +11 -12 ± 15 MeV/c 2 ● Signifjcance > 12σ ● PRL 115, 222002 (2015) 21 Image from XYZ states at the BESIII experiment by Gianfranco Morello Charm + XYZ at BES-III

  22. Z c states at BESIII Z c (4020) + e + e - → π + π - h c ● M = (4022.9 ± 0.8 ± 2.7) MeV/c 2 ● Γ = (7.9 ± 2.7 ± 2.6) MeV/c 2 ● Signifjcance > 8.9σ Isospin triplet PRL 111, 242001(2013) e + e - → π 0 π 0 h c Z c (4020) 0 ● M = 4023.9 ± 2.2 ± 3.8 MeV/c2 ● Γ fjxed to Z c (4020) + ● Signifjcance: 5σ PRL 113, 212002(2014) 22 Charm + XYZ at BES-III

  23. Z c states at BESIII In e + e - → π + (D * D * ) - Z c (4025) + ● M = (4026.3 ± 2.6 ± 3.7) MeV/c 2 ● Γ = (24.8 ± 5.6 ± 7.7) MeV/c 2 ● Signifjcance > 10σ Isospin triplet Z c (4025) 0 ● M = (4025.5 +2.0 -4.7 ± 3.1) MeV/c 2 ● Γ = (23.0 ± 6.0 ± 1.0) MeV/c 2 ● Signifjcance > 5.9σ PRL112, 132001 (2014) 23 Charm + XYZ at BES-III

  24. Z c states at BESIII: Summary Table by Guangshun Huang «Overview of the BESIII Experiment» 4th LNF Workshop on Cylindrical GEM Detectors 24 Charm + XYZ at BES-III

  25. X States at BESIII X(3872) e + e - → γX(3872) X(3872) → π + π - J/ψ 6.3σ M = 3871.9 ± 0.7 ± 0.2 MeV/c 2 ● Γ < 2.4 MeV/c 2 @ 90% C.L ● Y(4260) → γX(3872) decay was recently observed at BESIII PRL 112, 092001 (2014) X(3823) X(3823) observed in e + e - → π + π - X(3823) X(3823)→γχ C1 M = 3821.9 ± 1.3 ± 0.7MeV/c 2 ● 6.2σ Consistent with ψ(1 3 D 2 ) ● PRL 115, 011803 (2015) 25 Charm + XYZ at BES-III

  26. Y States Y(4230) PRL, 114, 092003 e + e - → ωχ c0 4.23 GeV M = 4230 ± 8 ± 6 MeV/c2 ● Γ = 38 ± 12 ± 2 MeV ● Signifjcance > 9σ ● 4.26 GeV Possible interpretations: ● Tetraquark ● ψ(4S) ● threshold effect? 26 Charm + XYZ at BES-III

  27. Summary ● Charm physics – Semileptonic analyses (hadronic FF and decay constant) ● D + → K - π + e + ν e, D 0 → K - /π - e + ν e , D + → ωe + ν e ● Recent progress in XYZ: – Neutral Z c partners are found: ● Z c (3900) 0 , Z c (3885) 0 , Z c (4020) 0 , Z c (4025) 0 ψ(1 3 D 2 ) (X(3823)) is observed – Y(4230) – ● BESIII continues to take data – More interesting results are expected soon 27 Charm + XYZ at BES-III

Download Presentation
Download Policy: The content available on the website is offered to you 'AS IS' for your personal information and use only. It cannot be commercialized, licensed, or distributed on other websites without prior consent from the author. To download a presentation, simply click this link. If you encounter any difficulties during the download process, it's possible that the publisher has removed the file from their server.

Recommend


More recommend